US6119523A - Method and apparatus for electronic compensation of erroneous readings caused by resonance in a capacitive pressure transducer - Google Patents
Method and apparatus for electronic compensation of erroneous readings caused by resonance in a capacitive pressure transducer Download PDFInfo
- Publication number
- US6119523A US6119523A US09/308,409 US30840999A US6119523A US 6119523 A US6119523 A US 6119523A US 30840999 A US30840999 A US 30840999A US 6119523 A US6119523 A US 6119523A
- Authority
- US
- United States
- Prior art keywords
- transducer
- resonance
- pressure transducer
- capacitive pressure
- compensation
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
- 238000000034 method Methods 0.000 title claims abstract description 17
- 238000005259 measurement Methods 0.000 claims abstract description 21
- 238000001514 detection method Methods 0.000 claims abstract description 5
- 230000004888 barrier function Effects 0.000 claims abstract description 4
- 239000012528 membrane Substances 0.000 claims description 34
- 230000003321 amplification Effects 0.000 claims description 3
- 230000001419 dependent effect Effects 0.000 claims description 3
- 238000003199 nucleic acid amplification method Methods 0.000 claims description 3
- 230000010355 oscillation Effects 0.000 claims description 3
- 230000001133 acceleration Effects 0.000 description 2
- 238000012544 monitoring process Methods 0.000 description 2
- 238000012546 transfer Methods 0.000 description 2
- 238000009530 blood pressure measurement Methods 0.000 description 1
- 239000003990 capacitor Substances 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000013461 design Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000012530 fluid Substances 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000003071 parasitic effect Effects 0.000 description 1
- 230000003068 static effect Effects 0.000 description 1
Images
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L9/00—Measuring steady of quasi-steady pressure of fluid or fluent solid material by electric or magnetic pressure-sensitive elements; Transmitting or indicating the displacement of mechanical pressure-sensitive elements, used to measure the steady or quasi-steady pressure of a fluid or fluent solid material, by electric or magnetic means
- G01L9/12—Measuring steady of quasi-steady pressure of fluid or fluent solid material by electric or magnetic pressure-sensitive elements; Transmitting or indicating the displacement of mechanical pressure-sensitive elements, used to measure the steady or quasi-steady pressure of a fluid or fluent solid material, by electric or magnetic means by making use of variations in capacitance, i.e. electric circuits therefor
Definitions
- the present invention concerns a method for measuring pressure using a capacitive pressure transducer and a pressure measuring device comprising a capacitive pressure transducer according to the preamble of claim 10.
- Capacitive pressure transducers are known from JP-A-04 104 027 and EP-A-0 194 953. The latter may also be used for measuring force or acceleration. Its properties are determined and resonance avoided during use.
- the purpose of the present invention is to remove the drawbacks of the prior art and to provide a method and device for measuring pressure where the influence of resonance in the capacitive pressure transducer is compensated.
- the invention is based on the concept of causing the capacitive pressure transducer to resonate, measuring the erroneous reading caused by the resonance and feeding a feedback compensation signal to the measuring element where the signal is essentially unfiltered.
- the device according to the invention is based on the concept of an apparatus for compensating effects of resonance comprising error detection and compensation elements whose upper barrier frequency is above the resonance frequency of the transducer, for detecting an erroneous reading of the transducer and for generating a compensation signal to be fed into the detection elements.
- the invention provides considerable benefits.
- the compensation is most efficient and, in the case of undistorted self-oscillation, it will eliminate the erroneous reading to 100%.
- FIG. 1 is a side view of the basic scheme of a capacitive pressure transducer that can be used in the invention
- FIG. 2 depicts a typical known measuring circuit for the pressure transducer of FIG. 1;
- FIG. 3 is a more detailed illustration of element F1 in FIG. 2;
- FIG. 4 depicts a coupling according to the invention for electronic compensation of erroneous readings caused by resonance in a capacitive pressure transducer.
- the type of pressure transducers described herein are generally called capacitance manometers.
- the pressure to be measured acts on one side of the membrane, whereas its other side is under a reference pressure which is usually very low.
- a capacitance manometer When pressure is measured exploiting the movements of the membrane even a number of parasitic parameters are generated which in no way contribute positively to the measurement.
- One of these parameters comprises the natural resonance frequency of the membrane. At this frequency the membrane self-oscillates with a minimum of external energy input. Based on mere intuition, it is obvious that such self-oscillation of the membrane will interfere with the measurement. On the basis of practical measurements it is also known that this is the case.
- FIG. 1 depicts the transducer element with membranes and current measuring electrodes.
- an electrode 4 has been arranged on its inner side in the reference vacuum space 3 and a second electrode 5 on the housing body 7 in the same space. Connecting wires 6 lead from these electrodes 4 and 5 to the outer side of the transducer housing.
- the membrane 2 is fixedly tensioned between the transducer housing 7 and the bottom part 8 by means of glass joints 9 and moves in toward the level of the transducer housing 7 under elevated pressure.
- the capacitance is inversely proportional to the distance of the electrodes and therefore also to the pressure.
- Cp is the capacitance between the electrodes 4 and 5 of the transducer element 1 in the capacitor according to FIG. 2 and thus, it represents the distance between these, said distance in turn being proportional to the pressure.
- a parallelogram signal having a frequency of 8 kHz (Q) feeds the two switches SW1 and SW2.
- Uk is a reference voltage which in reality is a parallelogram signal having the same frequency as Q and having a constant amplitude.
- the output signal is proportional to the reference voltage Uk ##EQU8## and the reference capacitance Cr and inversely proportional to the measured capacitance.
- the output signal is proportional to the distance between the electrodes wherefore it is also proportional to the pressure.
- the membrane is shifted in relation to the pressure, whereby the distance between the electrodes is altered resulting in altered capacitance.
- the oscillation is damped and occurs at the resonance frequency of the membrane. If force is instead introduced in the form of pulses or waves in the material having the same frequency as the resonance frequency of the membrane, the self-oscillation is increased and then maintained constant at a certain amplitude where the introduced energy and energy losses are the same. In connection with this type of membrane movement (resonance) the amplitude can become great and even exceed the entire normal measurement range. In spite of this circumstance the membrane still measures the static pressure of the gas in front of the membrane. However, a positive deviation is now added to the measurement result, the deviation being proportional to the quadrature of the amplitude of the self-oscillation.
- Us will not be equal to Uk at the resonance frequency but will instead vary proportional to the capacitance.
- the relation is the same as in the previous case.
- Us can be separated by measuring the difference between Us and Uk by means of a circuit whose barrier frequency is clearly beyond the resonance frequency.
- Us is a sinusoidal voltage with the resonance frequency of the membrane. This alternating voltage is amplified, rectified, filtered and scaled for returning to the summing point between R2 and R3.
- FIG. 4 shows the circuit in practice.
- the signal Us is compared to Uk between the resistances R4 and R5 and is then amplified.
- the signal is rectified by the diode D and is filtered by the low-pass filter F4, and at the output phase offset is adjusted by F5, whereafter the output voltage Ures is fed back to the nodal point between R2 and R3 via a resistor R res .
- the compensation takes place such that the membrane is caused to resonate by means of a variable tone generator.
- the erroneous reading of the output signal is recorded during resonance as compared to non-resonance.
- the signal Ures from the compensation circuit is switched and scaled until no difference between Uut during resonance and non-resonance is measurable.
- the compensation is very efficient and, in the case of undistorted self-resonance, able to eliminate the erroneous reading to 100%. This can be done during calibration of the transducer.
- Resonance problems of this type can occur in certain systems due to unsuccessful coaction of vibrations from pumps and the system design.
- the compensation circuit is in such case a must if measurements are to be performed. Often the resonance in such cases tends to be variable in time and size, wherefore the output signal without compensation varies in the second power in view of these error sources in a most disturbing ripple.
- the measurement signal can be rectified by quadration.
- a rectifier can even be used which generates a voltage that is a function of the amplitude of the membrane oscillation.
- the measurement error can also be made modulation dependent in the desired manner by varying the amplification prior to the rectifier and by varying the degree of modulation where the error is zero.
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Fluid Pressure (AREA)
- Control Of Motors That Do Not Use Commutators (AREA)
- Measurement Of Resistance Or Impedance (AREA)
- Filters And Equalizers (AREA)
Applications Claiming Priority (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| FI965016 | 1996-12-13 | ||
| FI965016A FI101018B (sv) | 1996-12-13 | 1996-12-13 | Förfarande och anordning för elektronisk kompensation av missvisning t ill följd av resonans hos en kapacitiv tryckgivare |
| PCT/IB1997/001562 WO1998026262A1 (en) | 1996-12-13 | 1997-12-12 | Method and apparatus for electronic compensation of erroneous readings caused by resonance in a capacitive pressure transducer |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| US6119523A true US6119523A (en) | 2000-09-19 |
Family
ID=8547270
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US09/308,409 Expired - Lifetime US6119523A (en) | 1996-12-13 | 1997-12-12 | Method and apparatus for electronic compensation of erroneous readings caused by resonance in a capacitive pressure transducer |
Country Status (7)
| Country | Link |
|---|---|
| US (1) | US6119523A (de) |
| EP (1) | EP0944817B1 (de) |
| JP (1) | JP2001506006A (de) |
| AT (1) | ATE213541T1 (de) |
| DE (1) | DE69710606T2 (de) |
| FI (1) | FI101018B (de) |
| WO (1) | WO1998026262A1 (de) |
Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7161476B2 (en) | 2000-07-26 | 2007-01-09 | Bridgestone Firestone North American Tire, Llc | Electronic tire management system |
| US20080184804A1 (en) * | 2004-12-27 | 2008-08-07 | Thales | Resonator Measurement Device and Method Employing the Device |
| US20110056302A1 (en) * | 2008-04-23 | 2011-03-10 | Nxp B.V. | Electronic circuit for controlling a capacitive pressure sensor and capacitive pressure sensor system |
| US20110215188A1 (en) * | 2010-03-04 | 2011-09-08 | Dispensing Dynamics International | Paper towel dispensing systems |
| US8266465B2 (en) | 2000-07-26 | 2012-09-11 | Bridgestone Americas Tire Operation, LLC | System for conserving battery life in a battery operated device |
| US20140260647A1 (en) * | 2013-03-13 | 2014-09-18 | Invensense, Inc. | Pressure sensor stabilization |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6837112B2 (en) * | 2003-03-22 | 2005-01-04 | Stec Inc. | Capacitance manometer having a relatively thick flush diaphragm under tension to provide low hysteresis |
| US7554343B2 (en) | 2005-07-25 | 2009-06-30 | Piezoinnovations | Ultrasonic transducer control method and system |
| KR101355098B1 (ko) | 2012-10-10 | 2014-02-04 | 주식회사 오토산업 | 용량성 압력센서의 출력제어회로 |
| JP6357090B2 (ja) * | 2014-12-02 | 2018-07-11 | 株式会社堀場エステック | 静電容量型センサ |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2578323B1 (fr) * | 1985-03-01 | 1987-11-20 | Metravib Sa | Capteur integre de grandeurs mecaniques a effet capacitif et procede de fabrication. |
| JP2905902B2 (ja) * | 1990-08-24 | 1999-06-14 | 横河電機株式会社 | 半導体圧力計およびその製造方法 |
-
1996
- 1996-12-13 FI FI965016A patent/FI101018B/sv not_active IP Right Cessation
-
1997
- 1997-12-12 EP EP97946004A patent/EP0944817B1/de not_active Expired - Lifetime
- 1997-12-12 JP JP52642498A patent/JP2001506006A/ja active Pending
- 1997-12-12 AT AT97946004T patent/ATE213541T1/de not_active IP Right Cessation
- 1997-12-12 DE DE69710606T patent/DE69710606T2/de not_active Expired - Lifetime
- 1997-12-12 US US09/308,409 patent/US6119523A/en not_active Expired - Lifetime
- 1997-12-12 WO PCT/IB1997/001562 patent/WO1998026262A1/en not_active Ceased
Non-Patent Citations (2)
| Title |
|---|
| Puers B et al. "a capacitive pressure sensor with low impedance output and active suppression of parasitic effects", sensors and actuators, vol. A21, No. 1/03, Feb. 1, 1990, pp. 108-114, XP000149570. |
| Puers B et al. a capacitive pressure sensor with low impedance output and active suppression of parasitic effects , sensors and actuators, vol. A21, No. 1/03, Feb. 1, 1990, pp. 108 114, XP000149570. * |
Cited By (11)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7161476B2 (en) | 2000-07-26 | 2007-01-09 | Bridgestone Firestone North American Tire, Llc | Electronic tire management system |
| US8151127B2 (en) | 2000-07-26 | 2012-04-03 | Bridgestone Americas Tire Operations, Llc | System for conserving battery life in a battery operated device |
| US8266465B2 (en) | 2000-07-26 | 2012-09-11 | Bridgestone Americas Tire Operation, LLC | System for conserving battery life in a battery operated device |
| US20080184804A1 (en) * | 2004-12-27 | 2008-08-07 | Thales | Resonator Measurement Device and Method Employing the Device |
| US7798005B2 (en) * | 2004-12-27 | 2010-09-21 | Thales | Resonator measurement device and method employing the device |
| US20110056302A1 (en) * | 2008-04-23 | 2011-03-10 | Nxp B.V. | Electronic circuit for controlling a capacitive pressure sensor and capacitive pressure sensor system |
| US8516894B2 (en) * | 2008-04-23 | 2013-08-27 | Nxp B.V. | Electronic circuit for controlling a capacitive pressure sensor and capacitive pressure sensor system |
| US20110215188A1 (en) * | 2010-03-04 | 2011-09-08 | Dispensing Dynamics International | Paper towel dispensing systems |
| US8511599B2 (en) | 2010-03-04 | 2013-08-20 | Richard LaLau | Paper towel dispensing systems |
| US20140260647A1 (en) * | 2013-03-13 | 2014-09-18 | Invensense, Inc. | Pressure sensor stabilization |
| US9880063B2 (en) * | 2013-03-13 | 2018-01-30 | Invensense, Inc. | Pressure sensor stabilization |
Also Published As
| Publication number | Publication date |
|---|---|
| WO1998026262A1 (en) | 1998-06-18 |
| EP0944817B1 (de) | 2002-02-20 |
| DE69710606T2 (de) | 2002-11-21 |
| ATE213541T1 (de) | 2002-03-15 |
| JP2001506006A (ja) | 2001-05-08 |
| EP0944817A1 (de) | 1999-09-29 |
| DE69710606D1 (de) | 2002-03-28 |
| FI101018B (sv) | 1998-03-31 |
| FI965016A0 (fi) | 1996-12-13 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| AS | Assignment |
Owner name: BALZERS AND LEYBOLD INSTRUMENTATION AB, FINLAND Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNORS:OLSSON, RAY;BJORKMAN, PER;REEL/FRAME:010129/0707 Effective date: 19990519 |
|
| STCF | Information on status: patent grant |
Free format text: PATENTED CASE |
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| FPAY | Fee payment |
Year of fee payment: 4 |
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